Study of optoelectronic and thermoelectric properties of BaSiO3 perovskite under moderate pressure for energy renewable devices applications

Strategies and challenges of high-pressure methods applied to thermoelectric materials

“…122 On the other hand, this example does experimentally verify that significant magneto-thermoelectric effects are possible only when the carrier mobilities are rather high, as follows from Eqs. (7) and (8). Therefore, one can surmise that highpressure magneto-thermoelectric effects may be relevant to highquality crystalline or 2D materials that are characterized by high carrier mobility, whereas the nanostructured and different composite materials that are commonly utilized in thermoelectric applications are unlikely to exhibit significant magneto-thermoelectric effects.…”

“…[1][2][3][4] At present, thermoelectric materials are widely used in cooling technologies, in energy-efficient motors in the automotive industry, in biomedicine (for example in biothermal batteries for powering pacemakers), in photovoltaics, and in various military, aerospace, and other applications. [5][6][7][8][9] To be competitive compared with other energy sources, thermoelectric devices should be characterized by high values of certain performance parameters, the most important of which is the dimensionless figure of merit ZT, defined as…”

Theoretical investigation of electronic, optical and thermoelectric properties of tellurium doped barium titanate (BTO) through modified Becke – Johnson exchange potential

“…[50]). The computed ε 1 (ω) increases from its static value and reaches maximum values at 4.4 eV and 4 eV for BaTiO 3 and Te -doped BaTiO 3 at 8.3%, where it exhibits plasmonic resonance [52]. Obviously, the peaks of maximum intensity are shifted towards lower energy region meaning that the light through Te -doped BaTiO 3 disperses more than BaTiO 3 because of longer wavelength [53].…”

Exploration of structural, electronic, optical, mechanical, thermoelectric, and thermodynamic properties of XInO 3 (X = As, Sb) compounds for energy harvesting applications

“…Like this, the cumulative measure of electrons and lattice vibrations is thermal conductivity (κ = κ l + κ e ). 55 Additionally, we can see individually calculated the electron and phonon thermal vibration by using the BoltzTrap and GIBB 2 software as depicted in Figure 5C,D. Thermal conductivity decreased by enhancing the temperature because of phonon vibrations is lessening against the temperature as compared to electron vibration in both compounds.…”